Properties of single Na+ channels in cut-open Myxicola giant axons

Time- and voltage-dependent behavior of the Na+ conductance in dialyzed intact Myxicola axons was compared with cut-open axons subjected to loose-patch clamp of the interior and to axons where Gigaseals were formed after brief enzyme digestion. Voltage and time dependence of activation, inactivation, and reactivation were identical in whole-axons and loose-patch preparations. Single channels observed in patch-clamp axons had a conductance of 18.3 +/- 2.3 pS and a mean open time of 0.84 +/- 0.12 ms. The time-dependence of Na+ currents found by averaging patch-clamp records was similar to intact axons, as was the voltage dependence of activation. Steady-state inactivation in patch-clamped axons was shifted by an average of 15 mV from that seen in loose-patch or intact axons. Substitution of D2O for H2O decreased single channel conductance by 24 +/- 6% in patch-clamped axons compared with 28 +/- 4% in intact axons, slowed inactivation by 58 +/- 8% compared with 49 +/- 6%, and increased mean open time by 52 +/- 7%. The results confirm observations on macroscopic channel behavior in Myxicola and resemble that seen in other excitable tissues.     

Localization of Nav1.7 in the normal and injured rodent olfactory system indicates a critical role in olfaction,pheromone sensing and immune function

Loss-of-function mutations in the pore-forming α subunit of the voltage-gated sodium channel 1.7 (Na_v1.7) cause congenital indifference to pain and anosmia. We used immunohistochemical techniques to study Na_v1.7 localization in the rat olfactory system in order to better understand its role in olfaction. We confirm that Na_v1.7 is expressed on olfactory sensory axons and report its presence on vomeronasal axons, indicating an important role for Na_v1.7 in transmission of pheromonal cues. Following neuroepithelial injury, Na_v1.7 was transiently expressed by cells of monocytic lineage. These findings support an emerging role for Na_v1.7 in immune function. This sodium channel may provide an important pharmacological target for treatment of inflammatory injury and inflammatory pain syndromes.     

Coupling of activation and inactivation gate in a K+‐channel: potassium and ligand sensitivity

Potassium (K⁺)‐channel gating is choreographed by a complex interplay between external stimuli, K⁺ concentration and lipidic environment. We combined solid‐state NMR and electrophysiological experiments on a chimeric KcsA–Kv1.3 channel to delineate K⁺, pH and blocker effects on channel structure and function in a membrane setting. Our data show that pH‐induced activation is correlated with protonation of glutamate residues at or near the activation gate. Moreover, K⁺ and channel blockers distinctly affect the open probability of both the inactivation gate comprising the selectivity filter of the channel and the activation gate. The results indicate that the two gates are coupled and that effects of the permeant K⁺ ion on the inactivation gate modulate activation‐gate opening. Our data suggest a mechanism for controlling coordinated and sequential opening and closing of activation and inactivation gates in the K⁺‐channel pore.     

Mechanism of Maxi-K Channel Activation by Dehydrosoyasaponin-I

Dehydrosoyasaponin-I (DHS-I) is a potent activator of high-conductance, calcium-activated potassium (maxi-K) channels. Interaction of DHS-I with maxi-K channels from bovine aortic smooth muscle was studied after incorporating single channels into planar lipid bilayers. Nanomolar amounts of intracellular DHS-I caused the appearance of discrete episodes of high channel open probability interrupted by periods of apparently normal activity. Statistical analysis of these periods revealed two clearly separable gating modes that likely reflect binding and unbinding of DHS-I. Kinetic analysis of durations of DHS-I-modified modes suggested DHS-I activates maxi-K channels through a high-order reaction. Average durations of DHS-I-modified modes increased with DHS-I concentration, and distributions of these mode durations contained two or more exponential components. In addition, dose-dependent increases in channel open probability from low initial values were high order with average Hill slopes of 2.4–2.9 under different conditions, suggesting at least three to four DHS-I molecules bind to maximally activate the channel. Changes in membrane potential over a 60-mV range appeared to have little effect on DHS-I binding. DHS-I modified calcium- and voltage-dependent channel gating. 100 nM DHS-I caused a threefold decrease in concentration of calcium required to half maximally open channels. DHS-I shifted the midpoint voltage for channel opening to more hyperpolarized potentials with a maximum shift of −105 mV. 100 nM DHS-I had a larger effect on voltage-dependent compared with calcium-dependent channel gating, suggesting DHS-I may differentiate these gating mechanisms. A model specifying four identical, noninteracting binding sites, where DHS-I binds to open conformations with 10–20-fold higher affinity than to closed conformations, explained changes in voltage-dependent gating and DHS-I-induced modes. This model of channel activation by DHS-I may provide a framework for understanding protein structures underlying maxi-K channel gating, and may provide a basis for understanding ligand activation of other ion channels.     

Dynamic compartmentalization of the voltage-gated sodium channels in axons

One of the major physiological roles of the neuronal voltage-gated sodium channel is to generate action potentials at the axon hillock/initial segment and to ensure propagation along myelinated or unmyelinated fibers to nerve terminal. These processes require a precise distribution of sodium channels accumulated at high density in discrete subdomains of the nerve membrane. In neurons, information relevant to ion channel trafficking and compartmentalization into sub-domains of the plasma membrane is far from being elucidated. Besides, whereas information on dendritic targeting is beginning to emerge, less is known about the mechanisms leading to the polarized distribution of proteins in axon. To obtain a better understanding of how neurons selectively target sodium channels to discrete subdomains of the nerve, we addressed the question as to whether any of the large intracellular regions of Nav1.2 contain axonal sorting and/or clustering signals. We first obtained evidence showing that addition of the cytoplasmic carboxy-terminal region of Nav1.2 restricted the distribution of a dendritic-axonal reporter protein to axons of hippocampal neurons. The analysis of mutants revealed that a di-leucine-based motif mediates chimera compartmentalization in axons and its elimination in soma and dendrites by endocytosis. The analysis of the others generated chimeras showed that the determinant conferring sodium channel clustering at the axonal initial segment is contained within the cytoplasmic loop connecting domains II-III of Nav1.2. Expression of a soluble Nav1.2 II-III linker protein led to the disorganization of endogenous sodium channels. The motif was sufficient to redirect a somatodendritic potassium channel to the axonal initial segment, a process involving association with ankyrin G. Thus, it is conceivable that concerted action of the two determinants is required for sodium channel compartmentalization in axons.     

The interaction of homologous series of alkanols with sodium channels in nerve membrane vesicles

Summary The potency of members of the homologous series of alkanols to block²²Na uptake through sodium channels stimulated by veratridine was studied in membrane vesicles obtained from lobster walking leg nerves. A cut-off was revealed at the level of 1-undecanol. However, secondary isomers of inactive primary homologues, such as 5-dodecanol and 5-tridecanol, were able to block ion flux. From the concentration required for an equipotent effect, it was calculated that the standard free energy for adsorption of primary alkanols is –725 cal/mol CH₂. Furthermore, since the concentration required for an equipotent effect for primary isomer was found to be lower than that obtained for secondary isomers, it is concluded that the latter are less potent than the former. The similarity between this set of results and those obtained in intact frog sciatic nerve (J. Requena et al.,J. Membrane Biol. 84:229–238, 1985) offers further support to the notion that the procedure employed to isolate the membrane vesicles does preserve the Na channels. However, the mechanism of alcohol inhibition of the Na channel in isolated membrane vesicles would seem to be somewhat different from that preferred in axons. While in vesicles the block needs to be thought in terms of a reduction in the number of conducting Na channel, in axons this is considered to be the less likely mode of action, mainly because under veratridine it is not possible to invoke a shift in the steady-state activation or inactivation.     

Inhibition of sodium currents by local anesthetics in chloramine-T- treated squid axons. The role of channel activation

In order to test the requirement of Na channel inactivation for the action of local anesthetics, we investigated the inhibitory effects of quaternary and tertiary amine anesthetics on normally inactivating and noninactivating Na currents in squid axons under voltage clamp. Either the enzymatic mixture pronase, or chloramine-T (CT), a noncleaving, oxidizing reagent, was used to abolish Na channel inactivation. We found that both the local anesthetics QX-314 and etidocaine, when perfused internally at 1 mM, elicited a "tonic" (resting) block of Na currents, a "time-dependent" block that increased during single depolarizations, and a "use-dependent" (phasic) block that accumulated as a result of repetitive depolarizations. All three effects occurred in both control and CT-treated axons. As in previous reports, little time-dependent or phasic block by QX-314 appeared in pronase-treated axons, although tonic block remained. Time-dependent block was greatest and fastest at large depolarizations (Em greater than +60 mV) for both the control and CT-treated axons. The recovery kinetics from phasic block were the same in control and CT-modified axons. The voltage dependence of the steady state phasic block in CT-treated axons differed from that in the controls; an 8-10% reduction of the maximum phasic block and a steepening and shift of the voltage dependence in the hyperpolarizing direction resulted from CT treatment. The results show that these anesthetics can bind rapidly to open Na channels in a voltage-dependent manner, with no requirement for fast inactivation. We propose that the rapid phasic blocking reactions in nerve are consequences primarily of channel activation, mediated by binding of anesthetics to open channels, and that the voltage dependence of phasic block arises directly from that of channel activation.     

Destruction of Sodium Conductance Inactivation in Squid Axons Perfused with Pronase

We have studied the effects of the proteolytic enzyme Pronase on the membrane currents of voltage-clamped squid axons. Internal perfusion of the axons with Pronase rather selectively destroys inactivation of the Na conductance (g_Na). At the level of a single channel, Pronase probably acts in an all-or-none manner: each channel inactivates normally until its inactivation gate is destroyed, and then it no longer inactivates. Pronase reduces _Na, possibly by destroying some of the channels, but after removal of its inactivation gate a Na channel seems no longer vulnerable to Pronase. The turn-off kinetics and the voltage dependence of the Na channel activation gates are not affected by Pronase, and it is probable that the enzyme does not affect these gates in any way. Neither the K channels nor their activation gates are affected in a specific way by Pronase. Tetrodotoxin does not protect the inactivation gates from Pronase, nor does maintained inactivation of the Na channels during exposure to Pronase. Our results suggest that the inactivation gate is a readily accessible protein attached to the inner end of each Na channel. It is shown clearly that activation and inactivation of Na channels are separable processes, and that Na channels are distinct from K channels.     

Molecular regions underlying the activation of low- and high-voltage activating calcium channels

We have studied two aspects of calcium channel activation. First, we investigated the molecular regions that are important in determining differences in activation between low- and high-voltage activated channels. For this, we made chimeras between the low-voltage activating Ca_V3.1 channel and the high-voltage activating Ca_V1.2 channel. Chimeras were expressed in oocytes, and calcium channel currents recorded by voltage clamp. For domain I, we found that the molecular region that is important in determining the voltage dependence of activation comprises the pore regions S5-P as well as P-S6, but surprisingly not the voltage sensor S1–S4 region, which might have been expected to play a major part. By contrast, the smaller, but still significant, modulating effects of domain II on activation properties were due to effects involving both S1–S4 and S5–S6 but not the I/II linker. Second, during channel activation we studied movement of the S4 segment in domain I of one of the chimeras, using cysteine-scanning mutagenesis. The reagent parachloromercuribenzensulfonate inhibited currents for mutants V263, A265, L266 and A268, but not for F269 and V271, and voltage dependence of inhibition for residue V263 indicated S4 movement, which occurred before channel opening. The data indicate movement outwards upon depolarisation so as to expose amino acids up to residue 268 in S4.Junying Li and Louisa Stevens contributed equally to this work.     

Regulation of the mechanosensitive cation channels by ATP and cAMP in leech neurons

Single-channel recordings were used to study the modulation of stretch-activated channels (SACs) by intracellular adenosine nucleotides in identified leech neurons. These channels exhibited two activity modes, spike-like (SL) and multiconductance (MC), displaying different polymodal activation. In the absence of mechanical stimulation, internal perfusion of excised patches with ATP induced robust and reversible activation of the MC but not of the SL mode. The ATP effect on channel activity was dose-dependent within a range of 1 μM-1 mM and was induced at different values of intracellular pH and Ca²⁺. The non-hydrolyzable ATP analog AMP-PNP, ATP without Mg²⁺ or ADP also effectively enhanced MC activity. Adenosine mimicked the effect of its nucleotides. At negative membrane potentials, both ATP and adenosine activated the channel. Moreover, ATP but not adenosine induced a flickering block. Addition of cAMP during maximal ATP activation completely and reversibly inhibited the channel, with activation and deactivation times of minutes. However, cAMP alone only induced a weak and rapid channel activation, without inhibitory effects. The expression of these channels in the growth cones of leech neurons, their permeability to Ca²⁺ and their sensitivity to intracellular cAMP are consistent with a role in the Ca²⁺ oscillations associated with cell growth.     

Sodium channel functioning based on an octagonal structure model

The complete amino acid sequence of a sodium channel from squid Loligo bleekeri has been deduced by cloning and sequence analysis of the complementary DNA. A unique feature of the squid sodium channel is the 1,522 residue sequence, approximately three-fourths of those of the rat sodium channels I, II and III. On the basis of the sequence, and in comparison with those of vertebrate sodium channels, we have proposed a tertiary structure model of the sodium channel where the transmembrane segments are octagonally aligned and the four linkers of S5–6 between segments S5 and S6 play a crucial role in the activation gate, voltage sensor and ion selective pore, which can slide, depending on membrane potentials, along inner walls consisting of alternating segments S2 and S4. The proposed octagonal structure model is contrasted with that of Noda et al. (Nature 320; 188–192, 1986). The octagonal structure model can explain the gating of activation and inactivation, and ion selectivity, as well as the action mechanism of both tetrodotoxin (TTX) and -scorpion toxin (ScTX), and can be applied not only to the sodium channel, but also to the calcium channel, potassium channel and cGMP-gated channel.The authors would like to express our cordial acknowledgments to Dr. Hideo Tani (Kowa) and Drs. Masahiko Fujino and Haruo Onda (Takeda Pharmaceutical) for their kind support for us to utilize their experimental facilities for DNA cloning and as well as for their stimulating and helpful discussions. We also thank Drs. Toshio Iijima, Michinori Ichikawa, Kiyonori Hirota, Messrs. Tadashi Kimura and Osamu Shono and all our colleagues (Supermolecular Science Division, Electrotechnical Laboratory) for their kind support to collect and isolate optic lobes from live squid. We greatly thank Professors Takuji Takeuchi (University of Tohoku) and David Landowne (University of Miami) for their illuminating discussions and valuable comments.     

Activation of squid axon K+ channels. Ionic and gating current studies

We have used data obtained from measurements of ionic and gating currents to study the process of K+ channel activation in squid giant axons. A marked improvement in the recording of K+ channel gating currents (IKg) was obtained by total replacement of Cl- in the external solution by NO-3, which eliminates approximately 50% of the Na+ channel gating current with no effect on IKg. The midpoint of the steady state charge-voltage (Qrel - V) relationship is approximately 40 mV hyperpolarized to that of the steady state activation (fo - V) curve, which is an indication that the channel has many nonconducting states. Ionic and gating currents have similar time constants for both ON and OFF pulses. This eliminates any Hodgkin-Huxley nx scheme for K+ channel activation. An interrupted pulse paradigm shows that the last step in the activation process is not rate limiting. IKg shows a nonartifactual rising phase, which indicates that the first step is either the slowest step in the activation sequence or is voltage independent. These data are consistent with the following general scheme for K+ channel activation: (formula; see text)     

Sodium channel activation mechanisms. Insights from deuterium oxide substitution.

Schauf and Bullock (1979. Biophys. J. 27:193-208; 1982. Biophys. J. 37:441-452), using Myxicola giant axons, demonstrated that solvent substitution with deuterium oxide (D2O) significantly affects both sodium channel activation and inactivation kinetics without corresponding changes in gating current or tail current rates. They concluded that (a) no significant component of gating current derives from the final channel opening step, and (b) channels must deactivate (during tail currents) by a different pathway from that used in channel opening. By contrast, Oxford (1981. J. Gen. Physiol. 77:1-22) found in squid axons that when a depolarizing pulse is interrupted by a brief (approximately 100 microseconds) return to holding potential, subsequent reactivation (secondary activation) is very rapid and shows almost monoexponential kinetics. Increasing the interpulse interval resulted in secondary activation rate returning towards control, sigmoid (primary activation) kinetics. He concluded that channels open and close (deactivate) via the same pathway. We have repeated both sets of observations in crayfish axons, confirming the results obtained in both previous studies, despite the apparently contradictory conclusions reached by these authors. On the other hand, we find that secondary activation after a brief interpulse interval (50 microseconds) is insensitive to D2O, although reactivation after longer interpulse intervals (approximately 400 microseconds) returns towards a D2O sensitivity similar to that of primary activation. We conclude that D2O-sensitive primary activation and D2O-insensitive tail current deactivation involve separate pathways. However, D2O-insensitive secondary activation involves reversal of the D2O-insensitive deactivation step. These conclusions are consistent with "parallel gate" models, provided that one gating particle has a substantially reduced effective valence.     

Differential effects of depolarization on the growth of crayfish tonic and phasic motor axons in culture

Previous studies have demonstrated neuron-specific differences in the inhibitory effects of depolarization upon neurite outgrowth. We examined whether there is a relationship between the normal impulse activity level of an axon and the effect of depolarization upon its growth. Inactive phasic motor axons and active tonic motor axons grow from crayfish abdominal nerve cord explants in culture. Depolarization of these axons with high K⁺ solutions produced greater inhibition of advancing growth cones from the phasic axons than from the tonic axons. During the period 20–40 min after the beginning of depolarization, tonic axon growth cones continued to advance, whereas phasic axon growth cones retracted. During chronic depolarization, all of the phasic axons retracted during the first day and approximately half of the phasic axons had degenerated after 4 days of depolarization. The majority of tonic axons continue to grow after 3 days of depolarization, and all of the tonic axon growth survived the 4 days of depolarization. The different responses of the growing phasic and tonic axons to depolarization appear to be Ca²⁺ dependent. The inhibitory effects of depolarization upon phasic axon growth were reduced by the Ca²⁺ channel blockers La³⁺ and Mg²⁺. Application of a Ca²⁺ ionophore, A23187, produces greater inhibition of phasic axon growth than tonic axon growth. This study demonstrates that depolarization produces greater inhibition of growth from inactive motor axons than from active motor axons. This is likely due to differences in Ca²⁺ regulation and/or sensitivity to intracellular Ca²⁺. © 1997 John Wiley & Sons, Inc. J Neurobiol 33: 85–97, 1997     

Modulation of the Kv1.3 Potassium Channel by Receptor Tyrosine Kinases

The voltage-dependent potassium channel, Kv1.3, is modulated by the epidermal growth factor receptor (EGFr) and the insulin receptor tyrosine kinases. When the EGFr and Kv1.3 are coexpressed in HEK 293 cells, acute treatment of the cells with EGF during a patch recording can suppress the Kv1.3 current within tens of minutes. This effect appears to be due to tyrosine phosphorylation of the channel, as it is blocked by treatment with the tyrosine kinase inhibitor erbstatin, or by mutation of the tyrosine at channel amino acid position 479 to phenylalanine. Previous work has shown that there is a large increase in the tyrosine phosphorylation of Kv1.3 when it is coexpressed with the EGFr. Pretreatment of EGFr and Kv1.3 cotransfected cells with EGF before patch recording also results in a decrease in peak Kv1.3 current. Furthermore, pretreatment of cotransfected cells with an antibody to the EGFr ligand binding domain (α-EGFr), which blocks receptor dimerization and tyrosine kinase activation, blocks the EGFr-mediated suppression of Kv1.3 current. Insulin treatment during patch recording also causes an inhibition of Kv1.3 current after tens of minutes, while pretreatment for 18 h produces almost total suppression of current. In addition to depressing peak Kv1.3 current, EGF treatment produces a speeding of C-type inactivation, while pretreatment with the α-EGFr slows C-type inactivation. In contrast, insulin does not influence C-type inactivation kinetics. Mutational analysis indicates that the EGF-induced modulation of the inactivation rate occurs by a mechanism different from that of the EGF-induced decrease in peak current. Thus, receptor tyrosine kinases differentially modulate the current magnitude and kinetics of a voltage-dependent potassium channel.     

Kv Channel S1-S2 Linker Working as a Binding Site of Human β-Defensin 2 for Channel Activation Modulation

Among the three extracellular domains of the tetrameric voltage-gated K⁺ (Kv) channels consisting of six membrane-spanning helical segments named S1–S6, the functional role of the S1-S2 linker still remains unclear because of the lack of a peptide ligand. In this study, the Kv1.3 channel S1-S2 linker was reported as a novel receptor site for human β-defensin 2 (hBD2). hBD2 shifts the conductance-voltage relationship curve of the human Kv1.3 channel in a positive direction by nearly 10.5 mV and increases the activation time constant for the channel. Unlike classical gating modifiers of toxin peptides from animal venoms, which generally bind to the Kv channel S3-S4 linker, hBD2 only targets residues in both the N and C termini of the S1-S2 linker to influence channel gating and inhibit channel currents. The increment and decrement of the basic residue number in a positively charged S4 sensor of Kv1.3 channel yields conductance-voltage relationship curves in the positive direction by ∼31.2 mV and 2–4 mV, which suggests that positively charged hBD2 is anchored in the channel S1-S2 linker and is modulating channel activation through electrostatic repulsion with an adjacent S4 helix. Together, these findings reveal a novel peptide ligand that binds with the Kv channel S1-S2 linker to modulate channel activation. These findings also highlight the functional importance of the Kv channel S1-S2 linker in ligand recognition and modification of channel activation.     

N-glycans modulate Kv1.5 gating but have no effect on Kv1.4 gating

Nerve and muscle action potential repolarization are produced and modulated by the regulated expression and activity of several types of voltage-gated K⁺ (K_v) channels. Here, we show that sialylated N-glycans uniquely impact gating of a mammalian Shaker family K_v channel isoform, K_v1.5, but have no effect on gating of a second Shaker isoform, K_v1.4. Each isoform contains one potential N-glycosylation site located along the S1-S2 linker; immunoblot analyses verified that K_v1.4 and K_v1.5 were N-glycosylated. The conductance-voltage (G-V) relationships and channel activation rates for two glycosylation-site deficient K_v1.5 mutants, K_v1.5^N290Q and K_v1.5^S292A, and for wild-type K_v1.5 expressed under conditions of reduced sialylation, were each shifted linearly by a depolarizing ∼ 18 mV compared to wild-type K_v1.5 activation. External divalent cation screening experiments suggested that K_v1.5 sialic acids contribute to an external surface potential that modulates K_v1.5 activation. Channel availability was unaffected by changes in K_v1.5 glycosylation or sialylation. The data indicate that sialic acid residues attached to N-glycans act through electrostatic mechanisms to modulate K_v1.5 activation. The sialic acids fully account for effects of N-glycans on K_v1.5 gating. Conversely, K_v1.4 gating was unaffected by changes in channel sialylation or following mutagenesis to remove the N-glycosylation site. Each phenomenon is unique for K_v1 channel isoforms, indicating that sialylated N-glycans modulate gating of homologous K_v1 channels through isoform-specific mechanisms. Such modulation is relevant to changes in action potential repolarization that occur as ion channel expression and glycosylation are regulated.     

A TEA-insensitive flickering potassium channel active around the resting potential in myelinated nerve

A novel potassium-selective channel which is active at membrane potentials between -100 mV and +40 mV has been identified in peripheral myelinated axons of Xenopus laevis using the patch-clamp technique. At negative potentials with 105 mM-K on both sides of the membrane, the channel at 1 kHz resolution showed a series of brief openings and closings interrupted by longer closings, resulting in a flickery bursting activity. Measurements with resolution up to 10 kHz revealed a single-channel conductance of 49 pS with 105 mM-K and 17 pS with 2.5 mM-K on the outer side of the membrane. The channel was selective for K ions over Na ions (PNa/PK = 0.033). The probability of being within a burst in outside-out patches varied from patch to patch (> 0.2, but often > 0.9), and was independent of membrane potential. Open-time histograms were satisfactorily described with a single exponential (tau o = 0.09 msec), closed times with the sum of three exponentials (tau c = 0.13, 5.9, and 36.6 msec). Sensitivity to external tetraethylammonium was comparatively low (IC50 = 19.0 mM). External Cs ions reduced the apparent unitary conductance for inward currents at Em = -90 mV (IC50 = 1.1 mM). Ba and, more potently, Zn ions lowered not only the apparent single-channel conductance but also open probability. The local anesthetic bupivacaine with high potency reduced probability of being within a burst (IC50 = 165 nM). The flickering K channel is clearly different from the other five types of K channels identified so far in the same preparation. We suggest that this channel may form the molecular basis of the resting potential in vertebrate myelinated axons.     

Cholinergic excitation of smooth muscles: Multiple signaling pathways linking M2 and M3 muscarinic receptors to cationic channels

Acetylcholine, the main neurotransmitter of the parasympathetic nervous system, depolarizes various smooth muscles and initiates their contraction via activating muscarinic cholinergic receptors. In most visceral smooth muscle tissues, such as the gastrointestinal tract, airways, and the urinary system, muscarinic receptors are comprised of predominant M₂ (about 80%)and minor M₃ (about 20%) subtypes. Cholinergic excitation is generally mediated by the opening of ion channels selective for monovalent cations (under physiological conditions, Na⁺ and K⁺); among them the cationic channel of an about 60 pS unitary conductance has been recently identified as the main target for acetylcholine action. The signal transduction leading to channel opening is very complex and involves activation of G_o protein (an M₂ effect), activation of phospholipase C (an M₃ effect), and [Ca²⁺]_i and voltage dependence of channel opening. These multiple signaling pathways were difficult to reconcile with the channel gating mechanisms since only a simplified two-state channel mechanism (e.g., one open and one shut state) was until recently available. However, our recent studies of channel gating in isolated outside-out membrane patches revealed a greater complexity. Thus, this cationic channel shows transitions between at least eight states, four open and four shut, with strong connections between adjacent shut and open states. Therefore, four pairs of connected states have been identified, which showed voltage-dependent transitions in each pair of shut/open states. Since the membrane potential did not affect the relative proportions between the pairs, we have assumed that these effects are controlled by ligands that bind to the channel and, thus, stabilize its various open conformations. In this work, direct tests of the above hypothesis have been performed, and their results showed that spontaneous brief channel gating exists in the absence of receptor or G-protein activation, which is strongly voltage-dependent (increasing at depolarized potentials). Furthermore, this activity was potentiated at a low agonist concentration, while channel openings generally remained brief. An increasing receptor occupancy by the agonist produced long channel openings, indicating a shift of gating towards a long open/brief shut pair of the channel states. These findings are interpreted in the context of the established signal transduction pathways;certain predictions for the whole-cell current are also examined.Neirofiziologiya/Neurophysiology, Vol. 36, Nos. 5/6, pp. 446–454, September–December, 2004.This revised version was published online in April 2005 with a corrected cover date and copyright year.     

Permeability of the squid giant axon to organic cations and small nonelectrolytes

Summary The permeability of the Na channel of squid giant axon to organic cations and small nonelectrolytes was studied. The compounds tested were guanidinium, formamidinium, and¹⁴C-labeled urea, formamide, thiourea, and acetone. Permeability was calculated from measurements of reversal potential and influx on internally perfused, voltage clamped squid axons. The project had two objectives: (1) to determine whether different methods of measuring the permeability of organic cations yield similar values and (2) to see whether neutral analogs of the organic cations can permeate the Na channel. Our results show that the permeability ratio of sodium to a test ion depends upon the ionic composition of the solution used. This finding is consistent with the view put forward previously that the Na channel can contain more than one ion at a time. In addition, we found that the uncharged analogs of permeant cations are not measurably permeant through the Na channel, but instead probably pass through the lipid bilayer.